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First analysis of the fully simulated channel. Marco Zanetti CMS Padova Muon Week – Bologna 10/4/2003. - PowerPoint PPT Presentation
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First analysis of the fully simulated channel
Marco ZanettiCMS Padova
Muon Week – Bologna 10/4/2003
WWH 0
Past analyses (e.g. M.Dittmar) have demostrated that this could be a very fast channel (with l , 5fb-1 ~ 1 month @ LL) for the discovery of the SM Higgs in the intemediate mass region 130< MH <2 MZ, filling the gap of
Because of the 2 impossible to distinguish a peak in the invariant mass distribution => not easy counting channel: => the precise knowledge of all possible backgrounds processes is fundamental;
Marco Zanetti CMS Padova
llllWWH 0
b
s
n
nS
)4( 0 lZZHBR
Marco Zanetti CMS Padova
Signal
x-sec (pb)events
in the sample
MH=120 0.036 9999
MH=140 0.114 9997
MH=160 0.182 9998
MH=200 0.104 9999
WWH 0Reference sample
WWnr is the main bkgr, with the same final states but reducible (next slides)
Marco Zanetti CMS Padova
sBackground
Process Ptmin x-sec (pb) N events L
5,5 77 17599 0.2 fb-1
(Pthard>20) 7,7 (1.4)·107 48471 3.5 nb-1
3,3 106 49489 49 nb-1
5,5 621 17991 29 pb-1
5,5 29, 12 36990 O( fb-1 )
WWqq
XZ */
Xtt
XZZZW ,
Xbb
Not yet considered:
• Single top ( )
• WWgg
XWtbpp
Marco Zanetti CMS Padova
Signal vs WWnr 1:
small |muons
Higgs produced mainly via g-g fusion (in 130< MH <2MZ 80% of the times)
WWnr produced by
z-boost
21
21
4 xx
xxz
z~1
z~10
WWnr evs more boosted along the beam
More isotropic signal muons spatial distribution
Marco Zanetti CMS Padova
Signal vs WWnr 1:
Could depend on PDF used, but no significant differences between
GRV94 (old) and CTEQ5L (DC04)
Di- system polar angle
8000 evsbarrel endcap
Marco Zanetti CMS Padova
Signal vs WWnr 2:
Signal:
Higgs scalar, W vectors => to have JTot=0 spin wave function must be:
nearby
LL
WW
TT
WW
TT
WWWW zzzzzz
z
)0()0()()()()(
3
1)0,0(
TL coupling not allowed
Case TT: each muon has the same SZ of the mother and must be produced with definite elicity => max prob to have emitted in the same direction
Case LL: not easy to demostrate that => again max prob to have emitted in the same direction
))((
WWnr:
Unpolarized initial state => TL coupling is allowed and @ MWW~160 half of the production rate
Case TL: no correlation in emission
Marco Zanetti CMS Padova
Signal vs WWnr 2:
Big difference in shape
Indipendece from the PDF
Implications also for MEt
opening angle
8000 evs
Marco Zanetti CMS Padova
Production chain
Pythia 6.158 (GRV94LO)
CMSIM 125
ORCA 6_2_3 (digi and reco)
Analysis
based on L3 reconstruction
Pile up
Marco Zanetti CMS Padova
HLT SelectionAlgorithmic Efficiency (Single+Di- standard sel. in |)
MH=120 MH=160 MH=200
L1 98.2% 99.2% 99.3%
L1+L2 95.0% 97.6% 98.1%
L1+L2+L3 91.1% 93.7% 96.3%
Analisys starting point: HLT Di- standard sel.
Eff (%) Rate (Hz) Events
Signal 80.6 2.3 ·10-4 8055
WWnr 72.8 1.1 ·10-3 12812
ZZ+WZ 77.6 2.0 ·10-3 28704
49.4 4.4 ·10-2 8888
Z/ 5.2 2.29 2574
28.1 1.81 13620
tt
bb
Signal overwhelmed (4 ord. mag.)
Marco Zanetti CMS Padova
Offline selections 1) Pt cut: Pt1,2 > 25,15; isolation @ 97% for both; opposite charge;
High eff. for the signal ~70%
Huge Rej. factor ( =Rbefore/Rafter) ~500 for sample; only 28 events survive
most of the * contribution suppressed
good Rej. (5) for thanks to isolation
bb
tt
2) Missing Et cut: MEt > 40 GeV;
Only 1 event survives (low pt s) with a integral rate of the same order of signal events (1.3·10-4 Hz)
Big Rej. (~21) for Z/
WWnr more rejected (2.1) than signal (1.3) as foreseen (spin correlation)
bb
Marco Zanetti CMS Padova
Offline selections
3) Invariant Mass cut: M < 70 GeV;
To reject events from Z peak;
I will select events with nearby muons:
M = {2|p1||p2|(1-cos)}1/2 => No lower bound
Rej. = 22.5 for Z/ sample; 3 events surving but with a integral rate greater than the signal (2.7·10-3 vs 1.3·1 0-4 Hz)
Big rejection also for WZ+ZZ
no more eventsbb
Marco Zanetti CMS Padova
Offline selections 4) Jet veto: rejected events with one jet with Et>20 in | ;
VETO REGION
Specific for top events (tt & Wtb)
Huge Rej. (~85) for ; only 5 events survive giving a smaller rate contribution than the signal (2.5·10-5 vs 4.7·10-5 Hz)
Much less effective for sample (if applied)
no more Z/ events
not so small rejection also for the signal (Rejec=2.7)
tt
bb
Marco Zanetti CMS Padova
Offline selections 5) Di- polar angle cut: => Di- System in the barrel8.0cos Di
Signal Rejec = 1.9 WWnr Reject = 2.4;
no more eventstt
6) Nearby s: < 0.8 &&< 1.5
Final plot
Eff.(%) Rate Rej
Signal 4.7 1.4·10-5 1.8 4.6
WWnr 0.5 7.9·10-6 3.3 10.5
WW+ZZ 0.003 0.7·10-6 3.1 30
N/1
Final numbers
Marco Zanetti CMS Padova
Statistical Results
MH=160 Nev @ 5fb-1 Nev @ 20fb-1
Signal 35 138
Background 22 88
7.4 14.7
Results for other masses:
Eff (%) @ 5fb-1 @ 20fb-1 L5(fb-1)
MH=120 1.9 0.5 1.1 390
MH=140 3.2 3.0 6.0 14
MH=200 2.7 2.5 4.9 21
MH=120: not viable; other H production processes like Vector Bosons Fusion can be used (CMS Note 2002/26: pp->jjH, H->WW->ll)
MH=200: different kinematic (e.g. no so effective spin correlation) different selections should be used
sample depleted at the very beginning of the offline selection
before beeing cut away, events give a integral rate contribution smaller than the signal and following cuts more effective to them than to signal ones.
Huge rejection for Z events by cuts 5 and 6 ( inizial state and muons back-to-back in transvers plane)
in the present Z/ sample not included qg->q(Z/) and => foreseen good rejection also by Jet veto
Marco Zanetti CMS Padova
Systematics
Statistics of the background samples used insufficient, anyway:
tt
bb
)/*( Zgqq
No effective contribution after offline selections
foreseen for these background processes
Marco Zanetti CMS Padova
DC04 Production
Xbb
XZ */
Sample Pt1 Pt2 M N events Rfin (Hz)
20 10 10 106 3·10-6
20 10 10 3·106 10-6
7 7 0 600K 2·10-7Xtt
95 % CL upper limit of Rate contribution after offline sel.if no events survive
WWnr sample: 200K events, Pt>7,7 => statistical error after offline selection %3/1 FinN
WZ ZZ samples: 200K +200Kevents, Pt>7,7 => statistical error after offline selection %9/1 FinN
(for tt forseen contribution O(10-6 Hz))
Marco Zanetti CMS Padova
Missing bkgr processes
WWgg
NLO process, x-sec 1 ord. smaller than WWnr; because of the gg inizial state should be taken into account.
Not yet implemented in Pythia. Not yet inculded in any analysis
XWtbpp x-sec ~ 0.5 and known to give a comparable contribution.
particularly dangerous, to be generated with CompHEP
tt
Wtbgg
(Stefano Marcellini)